The kinetics of the alkaline dissociation of myosin.

The rates of two processes in alkaline (pH 10.5–11.5) myosin solutions at 0 °C have been investigated: production of ionized tyrosine residues and production of light subunits. The progressive absorbance change is shown to result from a first-order irrevocable exposure to solvent and subsequent ionization of 40% of the tyrosine residues. Extrapolation to zero time gives the spectrophotometric ionization curve for native myosin; the pK of the abnormal tyrosines exceeds 12. Similarly, extrapolation to infinite time gives the curve for denatured myosin; the pK of the normal tyrosines (and of all tyrosines after denaturation) is 11.0–11.6. From the pH dependence of the rate, it is found that activation requires ionization of six residues and that their pK is much greater than 11.3. The rate of production of subunits was determined by fractionating the reaction mixture and determining the weight of light subunits produced. The process is also first order. Within experimental error, the rate constants for these two processes are equal. We conclude that they have the same rate-determining step. The data are consistent with either of two simple possible mechanisms. These are a rapid conformation change, followed by rate-determining subunit dissociation, followed by a rapid, irrevocable conformation change; or, a rapid conformation change, followed by a rate-determining, irrevocable conformation change, followed by rapid subunit dissociation.     

Electric birefringence of myosin subfragments.

Electric birefringence measurements have been made on aqueous solutions of myosin subfragments, heavy meromyosin, subfragments 1 and 2 (S-1 and S-2). All of these showed positive electric birefringence. Heavy meromyosin and S-2 showed a large intrinsic Kerr constant. From the analysis of the build up and decay process of the birefringence, the contribution of the slow induced dipole moment was concluded in heavy meromyosin and S-2, although the existence of the permanent dipole moment was not completely excluded. The decay process of the birefringence of heavy meromyosin was found to consist of two components; the fast one of which had a relaxation time of the same order as that of S-1. This is probably due to the presence of a flexible hinge in heavy meromyosin.     

Interaction of myosin subfragments with F-actin.

The effect of ionic strength, temperature, and divalent cations on the association of myosin with actin was determined in the ultracentrifuge using scanning absorption optics. The association constant (Ka) for the binding of heavy meromyosin (HmM) to F-actin was 1 X 10(7) M-1 at 20 degrees C, in 0.10 M KCl, 0.01 M imidazole (pH 7.0), 5 MM potassium phosphate, 1 mM MgCl2, and 0.3 mM ethylene glycol bis(beta-aminoethyl ether)-N,N'-tetraacetic acid. Ka was the same for HMM prepared by trypsin or chymotrypsin. The affinity of subfragment 1 (S1) for actin under the same ionic conditions was 3 X 10(6) M-1. Varying the preparative procedure for S1 had little effect on Ka. The small difference in binding energy between HMM and S1 suggests that either only one head can bind strongly to actin at a time or that free energy is lost during the sterically unfavorable attachment of the two heads to actin.     

Electric birefringence of myosin subfragments

Electric birefringence measurements have been made on aqueous solutions of myosin subfragments, heavy meromyosin, subfragments 1 and 2 (S-1 and S-2). All of these showed positive electric birefringence. Heavy meromyosin and S-2 showed a large intrinsic Kerr constant. From the analysis of the build up and decay process of the birefringence, the contribution of the slow induced dipole moment was concluded in heavy meromyosin and S-2, although the existence of the permanent dipole moment was not completely excluded. The decay process of the birefringence of heavy meromyosin was found to consist of two components; the fast one of which had a relaxation time of the same order as that of S-1. This is probably due to the presence of a flexible hinge in heavy meromyosin.     

Interaction of AMP-aminohydrolase with myosin and its subfragments.

We have shown that purified rabbit skeletal muscle AMP-aminohydrolase binds to rabbit muscle myosin, heavy meromyosin, and Subfragment 2 but does not bind to light meromyosin nor to Subfragment 1. The dissociation constant for binding to myosin was determined to be 0.14 muM. A new sedimentation boundary, presumably reflecting formation of a complex between AMP-aminohydrolase and heavy meromyosin or Subfragment 2, can be observed using the analytical ultracentrifuge. Binding of AMP-aminohydrolase to myosin, heavy meromyosin, or Subfragment 2 is abolished by phosphate (less than 10 mM), an inhibitor of AMP-aminohydrolase. No other rabbit muscle enzyme tested showed any interaction with myosin under the same conditions and there was no indication of complex formation between AMP-aminohydrolase and phosphofructokinase or phosphocreatine kinase in the analytical ultracentrifuge.     

The mechanism of regulatory light chain dissociation from scallop myosin.

The dissociation of the regulatory light chains from scallop myosin subfragments, on addition of EDTA, was investigated by using the fluorophore 8-anilinonaphthalene-1-sulphonate as a probe. The rate of this process (0.014 s-1) was partially limited by the rate of Mg2+ dissociation (0.058 s-1) from the non-specific high-affinity site. The dissociation of the regulatory light chain subfragment 1 was less extensive than from heavy meromyosin. Reassociation of the scallop regulatory light chain was induced on addition of Mg2+, but it appeared to be limited by a first-order step. The nature of this step was revealed by the kinetics of Mercenaria regulatory light chain association. Scallop heavy meromyosin, denuded of its regulatory light chains, exists in a refractory state, whose reversal to the nascent state limits the rate of light chain association (0.006 s-1). The formation of the refractory state is the driving force for the net dissociation of regulatory light chains from scallop heavy meromyosin. This mechanism is discussed with reference to existing structural information on light-chain-denuded myosin.     

Interaction of acetazolamide and 4-nitrothiophenolate ion with bivalent metal ion derivatives of bovine carbonic anhydrase.

The stability and rate constants for the interaction of acetazolamide (diamox) and 4-nitrothiophenolate ion (NTP) with the bivalent Mn, Co, Ni, Cu and Cd forms of bovine carbonic anhydrase have been measured by utilizing the distinct visible spectra of each metalloenzyme-NTP adduct. Differing stabilities of the various NTP and (particularly) diamox complexes reside mainly in varying values for the dissociation rate constants (kd). Intrinsic formation rate constants (for the acid form of the enzyme reacting with the basic form of the ligand) are uniformly high (greater than or equal 2 X 10(7) M-1 s-1 at 25 degrees C). Invariance of kd with pH and a bell-shaped log K-pH profile with the Cu-enzyme adducts are features observed previously with the native enzyme. Binding of NTP with the Cu and Cd metalloenzymes is stronger than to the native form.     

Magnesium regulates ADP dissociation from myosin V

Processivity in myosin V is mediated through the mechanical strain that results when both heads bind strongly to an actin filament, and this strain regulates the timing of ADP release. However, what is not known is which steps that lead to ADP release are affected by this mechanical strain. Answering this question will require determining which of the several potential pathways myosin V takes in the process of ADP release and how actin influences the kinetics of these pathways. We have addressed this issue by examining how magnesium regulates the kinetics of ADP release from myosin V and actomyosin V. Our data support a model in which actin accelerates the release of ADP from myosin V by reducing the magnesium affinity of a myosin V-MgADP intermediate. This is likely a consequence of the structural changes that actin induces in myosin to release phosphate. This effect on magnesium affinity provides a plausible explanation for how mechanical strain can alter this actin-induced acceleration. For actomyosin V, magnesium release follows phosphate release and precedes ADP release. Increasing magnesium concentration to within the physiological range would thus slow both the ATPase activity and the velocity of movement of this motor.     

ATPase activities and actin-binding properties of subfragments of Acanthamoeba myosin IA

Previous studies had led to the conclusion that the globular, single-headed myosins IA and IB from Acanthamoeba castellanii contain two actin-binding sites: one associated with the catalytic site and whose binding to F-actin activates the Mg2+-ATPase activity and a second site whose binding results in the cross-linking of actin filaments and makes the actin-activated ATPase activity positively cooperative with respect to myosin I concentration. We have now prepared a 100,000-Da NH2-terminal peptide and a 30,000-Da COOH-terminal peptide by alpha-chymotryptic digestion of the myosin IA heavy chain. The intact 17,000-Da light chain remained associated with the 100,000-Da fragment, which also contained the serine residue that must be phosphorylated for expression of actin-activated ATPase activity by native myosin IA. The 30,000-Da peptide, which contained 34% glycine and 21% proline, bound to F-actin with a KD less than 0.5 microM in the presence or absence of ATP but had no ATPase activity. The 100,000-Da peptide bound to F-actin with KD = 0.4-0.8 microM in the presence of 2 mM MgATP and KD less than 0.01 microM in the absence of MgATP. In contrast to native myosin IA, neither peptide cross-linked actin filaments. The phosphorylated 100,000-Da peptide had actin-activated ATPase activity with the same Vmax as that of native phosphorylated myosin IA but this activity displayed simple, noncooperative hyperbolic dependence on the actin concentration in contrast to the complex cooperative kinetics observed with native myosin IA. These results provide direct experimental evidence for the presence of two actin-binding sites on myosin IA, as was suggested by enzyme kinetic and filament cross-linking data, and also for the previously proposed mechanism by which monomeric myosins I could support contractile activities.     

Substructure of the myosin molecule: IV. Interactions of myosin and its subfragments with adenosine triphosphate and F-actin

The enzymic activity of several single-headed subfragments of myosin (HMM S-1 and single-headed HMM) has been compared to the double-headed derivative of myosin (HMM) both in the presence and absence of aetin. Under the assay conditions of our experiments, we find that HMM hydrolyses ATP at approximately twice the rate of any single-headed species. These results suggest a relatively independent functional role for each of the two heads of the myosin molecule.An attempt has been made to determine the stoichiometry of association between subfragments and actin, either in the absence of nucleotide or during the hydrolysis of ATP. It was originally thought that a comparison of the maximum turnover rate of HMM at infinite concentrations of actin with the maximum rate at infinite concentrations of enzyme (but with a fixed amount of actin) would yield the combining ratio of actin to HMM. However, the considerable variation of ATP turnover rates with the conditions of the experiment has made it impossible to reach any firm conclusions regarding stoichiometry. A more direct approach to the question of stoichiometry is possible in the absence of ATP. By reacting varying amounts of F-actin with a given concentration of subfragment and centrifuging the resulting complex, it is possible to determine the unbound concentration of subfragment in the supernatant. These data provide sufficient information to construct a Scatchard plot and show that twice as many moles of actin are bound by HMM as by HMM S-1. Furthermore, the association constant of actin for HMM is several orders of magnitude higher than that for the single-headed species.In connection with the question of why myosin has two “heads”, we have examined the ability of single-headed molecules to undergo the phenomenon of “superprecipitation”. We find that single-headed myosin (the preparation of which was discussed in the preceding paper) is able to superprecipitate in much the same manner as native myosin.We conclude from these studies that each head of the myosin molecule is able to function in a relatively independent fashion. These studies do not, of course, exclude the possibility of more subtle interactions between the heads of myosin which our techniques are not able to detect.